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Heat and mass transfer effects in direct methanol fuel cell: 1D model

dc.contributor.authorPinto, A. M. F. R.
dc.contributor.authorFalcão, D. S.
dc.contributor.authorOliveira, V. B.
dc.contributor.authorRangel, C. M.
dc.date.accessioned2010-07-07T15:05:55Z
dc.date.available2010-07-07T15:05:55Z
dc.date.issued2007
dc.description.abstractModels play an important role in fuel cell development since they facilitate a better understanding of parameters affecting the performance of fuel cells and fuel cells systems. In this work, a steady state, one-dimensional model accounting for coupled heat and mass transfer, along with the electrochemical reactions occurring in the DMFC is presented. The model accounts for the kinetics of the multi-step methanol oxidation at the anode while the kinetics of the cathodic oxygen reduction is modelled using the Tafel equation. Two-phase flow effects are neglected. The anode and cathode flow channels are treated using the continuous stirred tank reactor (CSTR) approach. The cell voltage expression incorporates the anodic and cathodic overpotentials as well as the ohmic losses across the membrane. The mixed potential of the cathode due to methanol crossover is also included. The reactions in the catalyst layers are considered homogeneous. Pressure gradients across the layers are assumed as negligible. Methanol and water transport through the membrane is assumed to be due to the combined effect of the concentration gradient and electro-osmotic force. Mass transport in the diffusion layers and membrane is described using effective Fick models. Local equilibrium at interfaces is represented by partition functions. The methanol flux in the cathode catalyst layer is considered as well as methanol crossover. The transport of heat through the gas diffusion layers is assumed to be a conduction-dominated process. The thermal conductivity for all the materials is assumed to be constant. Heat generation is considered in the catalyst layers. The analytical solutions for concentration and temperature across the cell are compared with recently data existing in literature and with in-house obtained results, for a wide range of operating conditions. The model shows very good agreement. This easily implemented simplified model is suitable for use in real-time DMFC simulationspt
dc.identifier.citationPinto, A. M. F. R.; Falcão, D. S.; Olveira, V. B.; Rangel, C. M. Heat and mass transfer effects in direct methanol fuel cell: 1D model. In: FUCE2007_0038, Tenth Grove Symposium, London, 2007pt
dc.identifier.urihttp://hdl.handle.net/10400.9/803
dc.language.isoengpt
dc.subjectRenewable hydrogenpt
dc.subjectMetal hydridespt
dc.subjectStand-alone systemspt
dc.titleHeat and mass transfer effects in direct methanol fuel cell: 1D modelpt
dc.typeconference object
dspace.entity.typePublication
oaire.citation.conferencePlaceLondonpt
oaire.citation.titleFUCE2007_0038, Tenth Grove Symposiumpt
person.familyNameRangel
person.givenNameCarmen M.
person.identifier.ciencia-idAA13-FF7C-9E29
person.identifier.orcid0000-0001-7996-8142
person.identifier.ridD-5477-2011
person.identifier.scopus-author-id7006108156
rcaap.rightsopenAccesspt
rcaap.typeconferenceObjectpt
relation.isAuthorOfPublication804e595a-d539-46a2-ae78-6cadc8ca9457
relation.isAuthorOfPublication.latestForDiscovery804e595a-d539-46a2-ae78-6cadc8ca9457

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